Pseudorotamers of Unconstrained Wittig Intermediates
J. Am. Chem. Soc., Vol. 120, No. 41, 1998 10655
a
1
Scheme 3. Pseudorotational Isomers of 3 and 5 and
resemblance of the essential H NMR data of oxaphosphetanes
Tentative Assignment of Rotamers A and B
3 and 5 (Table 3) suggests that the ethyl group in the rotamers
of 5 is also in the equatorial position. Accordingly, pseudoro-
tation between the diastereomeric syn/anti-Et,Me isomers is
proposed (Scheme 3). The equatorial Et positions of 3 and 5
parallel the equatorial Me groups observed for the dominating
1
,2-oxaphosphetane rotamers 1 and 1′ (Scheme 1), the pseu-
dorotation of which is still fast at -83 °C and rotamers have
1
not been resolved (averaged JC,P ) 96.4 Hz, Table 4), and for
their dibenzophosphole (DBP) analogues 8a (slow exchange at
1
-
53 °C: JC,P ) 98.1 Hz), which show coalescence of the C3
8
a
methylene protons near room temperature. With the help of
1
9
31
the coalescence criterion, we have calculated P coalescence
temperatures of -89 and -92 °C for 3 and 5, respectively.
The rotamers A of 3 and 5 dominate at low field in the 31P
spectra. Only a tentative assignment of A and B to the syn
and anti rotamers can be made according to Scheme 3, since
neither any relevant J coupling constants from H or
spectra nor any NOE enhancements in the H spectra are
accessible. Force field geometry optimizations, however,
a
Cy ) cyclohexyl. Only the 3S,4R- and 3R,4R pair, respectively,
are shown.
A B
Table 1. Pseudorotation Rate Constants k and k
(10 s-1, A is
3
A
the Main Isomer) and Population of A (p ) of 3 and 5 (T in °C)
3
1
13
C
3
5
20
21
1
2
2
T
k
A
k
B
p
A
k
A
k
B
p
A
2
3
starting from 50-100 conformations (generated by random
walk) to avoid local minima, suggest assigning the major
rotamers A to the 3-anti and 5-syn pairs: the calculated energy
-
95
90
85
80
75
70
50
0.284
0.667
1.64
0.986 0.776
1.06
2.51
5.40
11.5
23.8
43.2
-
-
-
-
-
-
-
2.23
5.32
11.06
0.770
0.764
0.759
3.51
-1
differences (3.1 kJ mol for 3 and 1.0 for 5) between syn and
anti pairs (3S,4R and 3R,4S of 3, 3R,4R and 3S,4S of 5) with
15.6
46.4
0.748
0.713
regard to trend correspond to the experimental energy differ-
599
q
-1
ences obtained from line-shape analysis (∆∆H of 1.8 kJ mol
30 1997
4960
for 3 and 0.6 for 5 (Table 2)).
Pseudorotation. From kinetic and thermodynamic arguments
it follows that the isomerizations of 1,2-oxaphosphetanes 3 and
1
withdrawing substituents on the P atom, JC3,P coupling constants
2
of 76-88 Hz have been reported.
1
13
From the JC,P coupling constants in CH3[ C]H2-labeled 3,
obtained with CH3[ C]H2I ( C ) 99.4%, Scheme 2), it is
deduced that in both rotamers of 3 the ethyl substituent is also
in the equatorial tbp position. The JC,P coupling constants at
110 °C are 106.8 Hz in the dominating (A at δC ) 35.6 ppm)
and 92.4 Hz in the minor rotamer (B at 21.5), both values being
in the typical range found for equatorial sp carbons. At -30
C an averaged value of 95.6 Hz (30.5 ppm) is observed. The
calculated population averaged value (pA ) 0.713, Table 1),
however, is 102.7 Hz. The difference of ca. 7 Hz could indicate
that the third rotamer with the ethyl group in apical tbp position,
7b,24
5
are the consequence of pseudorotations in turnstile
or
13
13
25
Berry permutation processes and not of acid-catalyzed ring
opening (“irregular process”
7b,24
via the protonated betaine).
1
First, isomerizations via the polar protonated betaines would
be expected to exhibit negative ∆S values due to the reduction
of freedom of the solvent induced by its reorientation toward
the polar protonated betaines. Second, the available acid
-
q
3
2,8b
26
°
(
19) Shanan-Atidi, H.; Bar-Eli, K. H. J. Phys. Chem. 1970, 74, 961-
9
63. Martin, M. L.; Delpuech, J.-J.; Martin, G. J. Practical NMR
Spectroscopy; Heyden & Son, Ltd.: London, 1980; pp 295-297.
1
(20) At -110 °C in the H spectrum, the lines are too broad, and in the
13
1
13
accessible C spectra, the concentrations are too low to observe H, C or
which is not populated to a detectable extent at low temperature,
even 13C, C J coupling constants in the rotamers of CH3[ C]H2-labeled
13
3
13
makes a minor contribution18 at temperatures above the fast
3.
exchange limit.
1
1
(
21) H, H-NOE enhancements have contributed to the identification of
8
b
1
It is reasonable to assume an analogous disposition of the
oxaphosphetane ring in the diastereomer 5, and the very close
the pseudorotamers of the dibenzophosphole-oxaphosphetane 8b. The H
lines of the oxaphosphetanes 3 and 5 at -90 to -110 °C, however, are too
broad for NOE experiments (and in part there is overlap of the relevant
1
(
16) All NMR data were taken in THF-d8, chemical shifts (δ, ppm)
relative to internal TMS ( H, C) and external 85% aqueous H3PO4 ( P),
coupling constants in hertz; for P data, see text. All H coupling patterns
have been analyzed by iteration with the program WIN-DAISY, Version
.0, Bruker-Franzen Analytik GmbH, Bremen, BRD, 1995.
17) Owing to the limited solubility of 6 and 7 and therefore relatively
resonances with cyclohexyl signals). For the same reasons H chemical shift
1
13
31
arguments, as applied to 8b, also cannot be used for 3 and 5. But the
3
1
1
1
following argument regarding the H chemical shifts observed at -30 °C
supports the tentative assignment. The only significant difference between
1
3
the H spectra of 3 and 5 is an upfield shift of 0.44 ppm observed for the
(
CH3-C4 group in 5 (1.21 and 0.77 ppm, respectively). Since the CH3-C4
groups in 3B and 5B clearly are positioned in the shielding region of the
equatorial free rotor P-phenyl substituent (force field geometry optimiza-
tions2 ), this upfield shift is likely to reflect the higher population of the
rotamer 5B compared to 3B (Table 1).
low concentrations of 3 (saturated and filtered solution, <49 mM) and 5 (7
1
3
mM), the essential C data have been obtained only for 3 at -30 °C, for
the dominating rotamer 3A at -100 °C (minor rotamer B not observable),
2,23
1
3
and for both rotamers of CH3[ C]H2-labeled 3 (20 mM) at -110 °C.
1
2
(
18) Assuming a typical apical coupling constant JC,P of 15 Hz, the
contribution of the population of the third rotamer at -30 °C would be ca.
%. Additional indications for a small contribution also come from small
differences between measured and calculated population averaged chemical
(22) For MM+ force fields in the program HyperChem 5.0 (Hypercube
Inc., Waterloo, Canada) the MM2 parameters and atom types (Allinger, N.
L., 1991) with the 1977 functional form (Allinger, N. L. J. Am. Chem. Soc.
1977, 99, 8127-8134. Burkert, U.; Allinger, N. L. Molecular Mechanics;
ACS Monograph 177; American Chemical Society: Washington, DC, 1982)
are used.
8
13
31
shifts of the ethyl-[ C]H2 group (30.5-31.6 ) 1.1 ppm) and of P (-65.6
3
1
-
(
-65.0 ) 0.6 ppm). Temperature effects on the P shifts are negligible
31
e.g., the P shift of 2 is constant from -110 to -30 °C within 0.1 ppm)
(23) In the program ChemPlus (Version 1.5, Hypercube Inc., Waterloo,
Canada), an Extension for HyperChem.
13
22
but cannot be excluded for C shifts because at low temperature a distinction
between temperature shifts and shifts which are due to observation of the
(24) Ramirez, F.; Ugi, I. AdV. Phys. Org. Chem. 1971, 9, 25-126.
17
dominating rotamer only (concentration of 3 too low to observe the minor
(25) Berry, R. S. J. Chem. Phys. 1960, 32, 933-938.
1
3
(26) As negative activation entropies (ca. -24 and -44 J mol K-1
)
-1
rotamer except its CH2 group in C-labeled 3) is impossible. Since the
third rotamer is not detectable at low temperature, a three-site exchange
analysis is not possible. Nevertheless, this uncertainty does not call into
question the principal results presented herein.
have been observed for the second step of the Wittig reaction, the first-
order thermolysis of the isolable oxaphosphetanes 9a5a and 9b, slightly
polar transition states have been postulated.
5b